Abstract

Using proton-proton collision data collected by the LHCb experiment at s=7 TeV, corresponding to an integrated luminosity of 1.0 fb−1, the ratio of branching fractions of the B0→D*−π+π−π+ decay relative to the B0→D*−π+ decay is measured to be B(B0→D*−π+π−π+)B(B0→D*−π+)=2.64±0.04(stat)±0.13(syst). The Cabibbo-suppressed decay B0→D*−K+π−π+ is observed for the first time, and the measured ratio of branching fractions is B(B0→D*−K+π−π+)B(B0→D*−π+π−π+)=(6.47±0.37(stat)±0.35(syst))×10−2. A search for orbital excitations of charm mesons contributing to the B0→D*−π+π−π+ final state is also performed, and the first observation of the B0→D¯1(2420)0π+π− decay is reported with the ratio of branching fractions B(B0→(D¯1(2420)0→D*−π+)π−π+)B(B0→D*−π+π−π+)=(2.04±0.42(stat)±0.22(syst))×10−2, where the numerator represents a product of the branching fractions B(B0→D¯1(2420)0π−π+) and B(D¯1(2420)0→D*−π+).Received 2 April 2013DOI:https://doi.org/10.1103/PhysRevD.87.092001This article is available under the terms of the Creative Commons Attribution 3.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.© 2013 CERN, for the LHCb Collaboration

Highlights

  • Open charm decays of b hadrons offer a means by which both the electroweak and QCD sectors of the Standard Model (SM) may be tested

  • Beyond measurements of CP violation and the phases derived from the CabibboKobayashi-Maskawa matrix, rare B ! DX decays may be used to search for new physics in decays mediated via annihilation or exchange processes

  • High-multiplicity B ! DX decays are receiving increasing attention at LHCb [1,2,3], in part owing to the large samples that can be obtained as a result of the copious bb" production at the LHC [4]

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Summary

INTRODUCTION

Open charm decays of b hadrons offer a means by which both the electroweak and QCD sectors of the Standard Model (SM) may be tested. The second measurement is of the ratio of branching fractions of the Cabibbo-suppressed (CS) decay B0 ! The first level of the trigger consists of a hardware stage that searches for either a large transverse energy cluster (ET > 3:6 GeV) in the calorimeters, or a single high-pT muon or dimuon pair in the muon stations This is followed by a software stage that applies a full event reconstruction. Candidate triple bachelors are formed from a þÀþ or KþÀþ combination, where all invariant mass values up to 3 GeV=c2 are accepted. Reconstructed B0 candidates are required to be well separated from the nearest PV, with decay time larger than 0.2 ps and good quality vertex fit. The total kinematic efficiency, kin, is determined from the simulation as the fraction of events that pass all reconstruction and selection requirements and the trigger. This fraction does not represent the true trigger efficiency, since it is evaluated with respect to a sample of events that have all passed the trigger

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